J. Mater. Sci. Technol. ›› 2021, Vol. 73: 165-170.DOI: 10.1016/j.jmst.2020.09.037
• Research Article • Previous Articles Next Articles
Zhipeng Longa, Qiuyue Jianga, Jiantao Wanga, Long Houa, Xing Yua, Yves Fautrelleb, Zhongming Rena, Xi Lia,b,*()
Received:
2020-05-07
Revised:
2020-06-07
Accepted:
2020-06-29
Published:
2021-05-20
Online:
2020-10-04
Contact:
Xi Li
About author:
*State Key Laboratory of Advanced Special Steels,Shanghai University, Shanghai 200072, China.E-mail address: lx_net@sina.com (X. Li).Zhipeng Long, Qiuyue Jiang, Jiantao Wang, Long Hou, Xing Yu, Yves Fautrelle, Zhongming Ren, Xi Li. Nucleation kinetics of paramagnetic and diamagnetic metal melts under a high magnetic field[J]. J. Mater. Sci. Technol., 2021, 73: 165-170.
Specimen | Impurity | Concentration (ppm) | Impurity | Concentration (ppm) |
---|---|---|---|---|
Pure aluminum | Ag, Sn, Na, Pb | ≤0.05 | Cr, Mn | ≤0.11 |
Ti, V, Ni, Zn | ≤0.32 | Mg, Si, Fe, Cu | ≤2.6 | |
Pure zinc | Ag, Ni, Co | ≤0.1 | Mg, Cu, In, Fe, As, Al | ≤0.5 |
Cd, Sn | ≤1.0 | Pb | ≤1.5 |
Table 1 Impurities in 5 N pure aluminum and pure zinc.
Specimen | Impurity | Concentration (ppm) | Impurity | Concentration (ppm) |
---|---|---|---|---|
Pure aluminum | Ag, Sn, Na, Pb | ≤0.05 | Cr, Mn | ≤0.11 |
Ti, V, Ni, Zn | ≤0.32 | Mg, Si, Fe, Cu | ≤2.6 | |
Pure zinc | Ag, Ni, Co | ≤0.1 | Mg, Cu, In, Fe, As, Al | ≤0.5 |
Cd, Sn | ≤1.0 | Pb | ≤1.5 |
Fig. 1. DTA curves of pure aluminum (a, c) and pure zinc (b, d) at different heating-cooling rates with and without a 12 T HMF. The solid lines, dash lines represent 0 T, 12 T HMF, respectively. (a, b) the melting endothermic curves; (c, d) the solidification exothermic curves.
Fig. 4. Plot of $\text{ln}\left( \beta /T_{\text{p}}^{2} \right)$ vs. 1/Tp using endothermic peak temperatures extracted from Figs. 1(a, b) and S1(a, b) in Supplementary Material under various HMFs. (a) pure aluminum; (b) pure zinc.
HMF intensities (T) | Slope | Activation energy ΔEa(105Jmol-1) | Nucleation work ΔGK(10-19Jmol-1) | |
---|---|---|---|---|
-ΔEa/R (K) | ΔGK/k (K) | |||
0 | -60749.10 ± 1439.21 | 11955.73 ± 814.20 | 5.0510 ± 0.1197 | 1.6499 ± 0.1124 |
4 | -60466.00 ± 1970.77 | 13476.76 ± 1140.40 | 5.0274 ± 0.1639 | 1.8598 ± 0.1574 |
8 | -60107.84 ± 4085.00 | 14509.46 ± 1997.47 | 4.9977 ± 0.3396 | 2.0023 ± 0.2757 |
12 | -59170.64 ± 2894.98 | 15348.15 ± 652.06 | 4.9197 ± 0.2407 | 2.1180 ± 0.8998 |
Table 2 Results of the slope for activation energy and nucleation work of pure aluminum extracted from Figs. 4(a) and 5 (a).
HMF intensities (T) | Slope | Activation energy ΔEa(105Jmol-1) | Nucleation work ΔGK(10-19Jmol-1) | |
---|---|---|---|---|
-ΔEa/R (K) | ΔGK/k (K) | |||
0 | -60749.10 ± 1439.21 | 11955.73 ± 814.20 | 5.0510 ± 0.1197 | 1.6499 ± 0.1124 |
4 | -60466.00 ± 1970.77 | 13476.76 ± 1140.40 | 5.0274 ± 0.1639 | 1.8598 ± 0.1574 |
8 | -60107.84 ± 4085.00 | 14509.46 ± 1997.47 | 4.9977 ± 0.3396 | 2.0023 ± 0.2757 |
12 | -59170.64 ± 2894.98 | 15348.15 ± 652.06 | 4.9197 ± 0.2407 | 2.1180 ± 0.8998 |
HMF intensities (T) | Slope | Activation energy ΔEa(105Jmol-1) | Nucleation work ΔGK(10-19Jmol-1) | |
---|---|---|---|---|
-ΔEa/R (K) | ΔGK/k (K) | |||
0 | -58677.11 ± 1675.29 | 11233.35 ± 1788.51 | 4.8787 ± 0.1393 | 1.5502 ± 0.2468 |
4 | -55253.51 ± 2981.68 | 12009.24 ± 1178.78 | 4.5941 ± 0.2479 | 1.6573 ± 0.1627 |
8 | -52875.43 ± 1633.61 | 14022.61 ± 2246.13 | 4.3963 ± 0.1358 | 1.9351 ± 0.3100 |
12 | -50334.43 ± 1930.34 | 14596.60 ± 1343.12 | 4.1851 ± 0.1605 | 2.0143 ± 0.1854 |
Table 3 Results of the slope for activation energy and nucleation work of pure zinc extracted from Figs. 4(b) and 5 (b).
HMF intensities (T) | Slope | Activation energy ΔEa(105Jmol-1) | Nucleation work ΔGK(10-19Jmol-1) | |
---|---|---|---|---|
-ΔEa/R (K) | ΔGK/k (K) | |||
0 | -58677.11 ± 1675.29 | 11233.35 ± 1788.51 | 4.8787 ± 0.1393 | 1.5502 ± 0.2468 |
4 | -55253.51 ± 2981.68 | 12009.24 ± 1178.78 | 4.5941 ± 0.2479 | 1.6573 ± 0.1627 |
8 | -52875.43 ± 1633.61 | 14022.61 ± 2246.13 | 4.3963 ± 0.1358 | 1.9351 ± 0.3100 |
12 | -50334.43 ± 1930.34 | 14596.60 ± 1343.12 | 4.1851 ± 0.1605 | 2.0143 ± 0.1854 |
Fig. 5. Plot of $\text{ln}\left[ \beta \left( 3{{T}_{\text{p}}}-{{T}_{\text{n}}} \right)/T_{\text{p}}^{2}{{\left( {{T}_{\text{n}}}-{{T}_{\text{p}}} \right)}^{3}} \right]$ vs. -1/Tp using exothermic peak temperatures extracted from Figs. 1(c, d) and S1(c, d) in Supplementary Material under various HMFs. (a) pure aluminum; (b) pure zinc.
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